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Equation 2 · The Arrow of Time and the Engine of Evolution

What does this equation mean?

Qmin⁡=kBTln⁡2Q_{\min} = k_{\mathrm{B}} T \ln 2

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Inputs and operationsk_B T ln 2
Result or conditionQ_min
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This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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Qmin⁡Q_{\min}

Symbol Q_min

QmQ_min is part of the quantity the equation computes from the expression on the right.

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kBk_{\mathrm{B}}

Symbol k_B

kBk_B is an input to the expression that computes the quantity on the left.

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TT

Symbol T

the temperature.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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How to interpret it

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What the article says around this equation

Writing a record redundantly is one thing; erasing one is a different, and thermodynamically cheaper to state, act. Rolf Landauer’s 1961 analysis established that any logically irreversible operation — one whose output does not determine a unique input, such as resetting a one-bit memory from either of two states to a single standard state — must, in an isothermal environment at temperature T , dissipate at least a fixed minimum quantity of heat to the surroundings: Qmin⁡=kBTln⁡2Q_{\min} = k_{\mathrm{B}} T \ln 2. per bit erased [ 3 ] . The bound follows from Liouville’s theorem: the phase-space volume corresponding to distinguishable logical states cannot be compressed into fewer accessible microstates without…
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Writing a record redundantly is one thing; erasing one is a different, and thermodynamically cheaper to state, act. Rolf Landauer’s 1961 analysis established that any logically irreversible operation — one whose output does not determine a unique input, such as resetting a one-bit memory from either of two states to a single standard state — must, in an isothermal environment at temperature T , dissipate at least a fixed minimum quantity of heat to the surroundings: Qmin⁡=kBTln⁡2Q_{\min} = k_{\mathrm{B}} T \ln 2. per bit erased [ 3 ] . The bound follows from Liouville’s theorem: the phase-space volume corresponding to distinguishable logical states cannot be compressed into fewer accessible microstates without exporting the corresponding entropy somewhere, and the only place available is heat expelled to the bath. It is a floor, not a typical value — Landauer’s own paper is explicit that real switching devices of his era dissipated many orders of magnitude more than this — but the floor is real and has since been demonstrated experimentally in isothermal single-bit erasure using exactly this publication’s kind of apparatus: a colloidal particle held in a modulated double-well potential.

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